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    13th

    World Conference on Earthquake EngineeringVancouver, B.C., Canada

    August 1-6, 2004Paper No. 3177

    NONLINEAR SEISMIC RESPONSE ANALYSIS OF

    PILE-SOIL-STRUCTURE INTERACTION SYSTEM

    WANG Feng-Xia1

    HE Zheng2

    OU Jin-Ping3

    SUMMARY

    In this paper, by using ANSYS

    software, a modified lumped-mass simplified nonlinear pile-soil-structure

    interaction (PSSI) model is established for shear-type RC frame structure under moderate and large

    earthquakes with rocking effect, dynamic nonlinearity of interaction between pile and soil, the contact

    state between pile and soil, raft and soil. Seismic response of a 4-storey building supported on piles is

    analyzed with respect to linear and nonlinear pile-soil systems using this model, and is compared with the

    behavior of buildings with rigid base under moderate and large earthquakes. A simplified model is

    presented to apply for the engineering applications.

    INTRODUCTION

    Under moderate and large earthquakes, the pile-soil-structure interaction (PSSI) system presents the

    evident nonlinear feature. In this case, it is necessary to take account of the nonlinearities induced in thesoil of the free field by seismic waves and of the additional nonlinear effects created by the structural

    vibrations.

    Approximate theories have to be used because the rigorous approach to the nonlinearity of pile-soil-

    structure system is difficult. Lumped-mass model proposed by Penzien[1]

    is a popular approximate

    method to solve the soil-structure interaction account for its convenient application to engineering

    practices.

    Many FEAsoftwares with the development of the computer technologies have been developed to the highquality engineering tools, which can be used to design, and analysis. Such as ANSYS

    , that can provide a

    common platform for fast, efficient analysis in a lot of important areas. Thus, the soil and structure

    interaction should utilize this effective tool, too.In this paper, a modified lumped-mass simplified model is established for shear-type RC frame structure

    under moderate and large earthquakes based on the Penzien, by using ANSYS software. Using this

    1PH.D. student, School of Civil Engineering, Harbin Institute of Technology, Harbin, China,

    email:[email protected]

    Associate Professor, School of Civil Engineering, Harbin Institute of Technology, Harbin, China,

    email:[email protected]

    Professor, School of Civil Engineering, Harbin Institute of Technology, Harbin, China,

    email:[email protected]

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    model, a 4-storey building supported on piles is analyzed with respect to linear and nonlinear pile-soil

    systems, and is compared with the behavior of buildings with rigid base under moderate and large

    earthquakes. Furthermore, the parametric influence of the system is studied. It suggests that the

    contact state of pile and soil changes from contact and slippage to separationunder seismic load,

    and the behavior of the building supported on a pile foundation is different from a rigid base.

    Moreover, the nonlinear seismic response of a building including the PSSI effect is differentfrom the linear response. The model built by ANSYS

    is easy to apply for the engineering

    applications.

    COMPUTATION MODEL AND PARAMETER DETERMINATION

    Computation model

    The hypotheses of the model are as follows: super-structure is simplified to shear-type RC frame structure,

    the pile group is assembled into single pile with the abilities of bending and shearing, and super-structure,

    piles and soil around piles present linear behavior, lateral soil resistance is nonlinear, furthermore, the

    contact nonlinear effect between piles and soil is taken into account.

    governing equationsIn present, Penzien model is one of soil-pile interaction system models widely used in practice, because it

    is simple and conceptual definitude. But this model does not consider the dynamic effect of soil around

    pile directly, and motion input is multi-points input format with different soil layer different motion input.

    The modified model takes account of several factors based on the Penzien model. First, free-field ground

    (soil around pile) simulated by PLANE element is considered into the model directly, and the viscous

    damping elements (COMBIN14) are set at the boundary of the free-field ground to simulate the radiation

    damping, thus motion input in this model can be input from the rock with the one motion input datum, so

    this model simplifies the computation process and presents dynamic interaction between the piles and soil

    factually. Second, pile is simulated by BEAM element and two vertical springs (CONTAC12) at the end

    of raft present the rocking effect. Third, using p-y curve simulates the nonlinear resistance between pile

    and soil, then the contact state of the interface between pile and soil is presented under dynamic load with

    contact elements,. The PSSI model is shown in Figure 1.

    The governing equations referred in [2] and [3] can be given as follows:

    Super-structure: (1)gx1MxKxCh)x(M rrrrrrr &&&

    &&&& =+++

    Figure 1. Simplified model of a pile-soil-structure

    system

    Super-structure

    Free-field

    Raft

    Pile

    Super-structure

    Radiation

    damping Soil Vertical

    spring

    with

    Bedrock

    gx&& gx&&

    Contact and nonlinear

    spring

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    Pile foundation: (2)

    Raft: (3)

    (4)

    Soil around pile: (5)

    In which the subscript r, p and s stand for superstructure, pile and soil, respectively; M, C and K arethe

    mass, damping and stiffness matrices, respectively; X, h and F are the displacement vector, floor height

    vector of super-structure and lateral soil resistance vector, respectively; m0,J0,, h and x0 are the mass, the

    moment of inertia, the rotation angle, the thickness and the relative displacement of the raft, respectively;

    f0 andMare the horizontal resistance and resistant moment of raft given by soil; hiis the distance from the

    floor to the raft; gx&& is the acceleration of motion input.

    Parameter determination

    Super-structure parameter

    Super-structure is simplified to shear-type structure, whose parameters determined according to the

    reference [4].

    The horizontal resistance and resistant moment of raft

    The horizontal resistance of raft is computed by the equation (6)

    (6)

    where k0 is the lateral soil resistant stiffness coefficient of the raft, which can be developed as

    (7)

    where bf0 is the computational width of the side of the raft, which is determined by the reference [5]; c0 is

    the damping factor; and m* is the resistance factor of the soil to raft, which is referred to the reference [6].

    The resistant moment of raft can be computed with equation (8)

    (8)

    wherecap

    K is the total rotational stiffness, can be determined by the reference [7]

    (9)

    where KRR is the rocking stiffness of a pile group, KRR=ri. iF , in which ri is distance between the

    center of rotation and the pile heads center, and Fi is the axial force at the pile heads, K is the

    rotational stiffness at the head of pile, when the heads of a pile group are the raft, the equation (9) can bemodified as equation (10).

    (10)

    where K is the rotational stiffness of the raft,)1(3

    8 30

    =

    GrK , 4 00

    4

    Ir = ,I0 is the moment of inertia of

    the raft, G is the shear module of soil, v is the Poisson s' ratio of soil.In this model, the rocking effect is simulated by the two vertical springs considering the contact influence

    between the raft and soil at the side of raft; the vertical spring stiffness can be developed as

    0)2

    ()( 0001

    =++++++=

    fh

    xxmxhxm ggin

    iriri

    &&&&&&&&&&&&

    2

    2*

    00

    hmbk f=

    cap

    KM=

    += KKK RRcap

    KKK RRcap

    +=

    gx&&&&& 1MFxKxCxM sssssss =++

    )()( 00000 ss xxcxxkf && +=

    gx&&&&& 1MFxKxCxM pPppPPP =+++

    02

    )2

    ()( 001

    0 =+++++++ =

    Mhh

    xxmxhxhmJ ggirin

    iiri

    &&&&&&&&&&&&&&

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    2

    R

    KK

    cap

    = (11)

    where R is the distance from the center of the raft to the side of the raft.

    Lateral soil resistant stiffness coefficient determination

    There are many methods to determine the lateral soil resistant stiffness coefficient, in which the mostcommonly used method to solve the nonlinear lateral soil resistance is p-y relation curve. Lateral loads on

    piles are resisted by the surrounding soil whose behavior is characterized by lateral soil resistance per unit

    length of pile, p, as a function of lateral displacement, y. The p-y relation is generally developed on the

    basis of a semi-empirical curve, which reflects nonlinear resistance of the local soil surrounding the pile at

    specified depth. The two most commonly used p-y models are those proposed by Matlock (1970) for soft

    clay and by Reese et al. (1974) for sand. In this paper, the p-y model proposed by Reese for sand is used to

    analysis the 4-storey building supported on piles. The parameter determination of p-y relation curve can be

    referred to the reference [6].

    PSSI system damping

    In the pile-soil-structure system, the damping includes two parts: the material damping and the radiation

    damping .The material damping is approximated with the Rayleigh approach. The damping matrix isC=aM+ K (12)

    where and are coefficients. The values ofa and are computed by using the first and second modalfrequencies (j=1 andj=2) with equation (13)

    )(2

    1

    2j

    j

    j

    +== (13)

    for the steel structure 1 = 2 =1%, and for the reinforced concrete structure 1 = 2 =5%. In this

    paper, the equivalent damping ratio [8] is taken as

    ~

    =

    +

    ++ )1(028.0

    2036.0

    ~)~

    ~1(

    ~

    2

    3

    3

    3

    2

    2

    2

    2

    hh

    ms

    s

    g

    ss

    (14)

    where ~ is the equivalent damping ratio; and g are the super-structure damping ratio and the material

    damping ratio of the soil; s and ~ are the first frequency of the super-structure and the PSSI system; s

    is the ratio of the stiffness of the super-structure to the soil, which is computed ass

    s

    v

    hs

    *= ; m is the

    mass ratio,3

    *

    a

    mm

    = ; h is the slenderness ratio,

    a

    hh

    *

    = ,and where h*and m* are the equivalent high

    and mass of the first mode shape of the super-structure, vs and are shear-wave velocity and the massdensity of the soil,a is the characteristic length of the bottom of the super-structure.The radiation damping which is simulated by the viscous damping elements (COMBIN14) set at the

    boundary of the free-field ground can be computed using equation (15) referred to the reference [9].'sc =aimsi (15)

    where msi is the mass of the soil layer; ai is valued according to the way proposed by Seed, ai= ii , in

    which i =0.05, and i =vsi/(2hsi), his is the thickness of the soil layer.

    BUILDING THE MODEL WITH ANSYS

    SOFTWARE

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    Choosing the element

    Using the before-mentioned method, the model is established by ANSYS

    software. Seven kinds of

    elements are used in this model, which are MASS21, COMBIN14, PLANE42, BEAM3, CONTAC12,

    COMBIN40 and LINK1 elements. MASS21 element is used to simulate the mass of the super-structure,

    and COMBIN14 element is used to simulate the stiffness of super-structure and the radiation damping at

    the boundary of the soil, and PLANE42 element is used to simulate the free-field soil and the raft, and

    BEAM3 element is used to simulate the pile, and CONTAC12 element with the contacting ability is usedto simulate the rocking spring of the side of raft, and COMBIN40 element with the contacting and

    nonlinear ability is used to simulate the nonlinear lateral soil resistance between the soil and pile. LINK1

    element is the dumb element to help simulate floors of the super-structure and the rocking effect.

    Building the model

    Building the model using ANSYS

    software includes two parts: building the geometric model and

    building the mechanical model. Building the geometric model uses the direct generation method to define

    the nodes and elements of a model directly on the basis of the geometric size. And then, the geometric

    model is turned into the mechanical model using constraint equations to establish the special associations

    among nodal degrees of freedom and applying the boundary condition to the model. The key problem in

    this model is how to simulate the rocking effect of the PSSI system, the actions referred [10] are shown in

    Figure 2. First, the cross point of the PLANE42 element simulating the raft, the BEAM element simulating

    the pile and the LINK1 element simulating the first floor of the superstructure is turned into rigid point

    using the following constraint equation in ANSYS

    format.

    CE,1,0,2,UY,1,1,UY,-1,3,ROTZ,-b (16)

    Then, the LINK1 elements simulating floors are coupled with the cross point using the constraintequations, so that the LINK1 elements simulating floors can keep the same rotation angle with the top of

    the BEAM3 element simulating the pile. The constraint equation of the LINK1 element simulating the

    first floor is as

    CE,2,0,3,UX,1,5,UX,-1,3,ROTZ,- h1 (17)

    In the same way, the constraint equations of the LINK1 elements simulating other floors can be generated

    in the similar form.

    Finally, the two vertical springs to simulate the rocking effect are set at the sides of the raft, with the

    constraint equation (18).

    Figure 2. Simulating to rocking effect

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    CE,4,0,8,UX,1,1,UX,-1 (18)

    In this way, the rocking effect can be simulated in the model by ANSYS

    software.

    ANALYTIC RESULT BY ANSYS

    SOFTWARE

    In this paper, the transient dynamic analysis (called time-history analysis) is used to analyze the seismic

    response of a 4-storey building supported on piles. In ANSYS software, three transient dynamic analysismethods are available: full, reduced and mode superposition, where the full solution method solves

    directly and needs no additional assumptions, and is suit to nonlinear problem.

    The input motion is the time history of the horizontal displacement and input from the bedrock at the

    bottom of the pile group.

    Computation model of a 4-storey frame supported on a pile group

    A 4-storey and 3-spans frame supported on a pile group with the raft is analyzed as a typical common

    structure in II site as shown in Figure 3, and the seismic fortification intensity of the building area is 8.

    The weight for the first and the forth floors is 1200kN, the weight for other floors is 1000kN; the first

    story stiffness is 0.544105

    kN/m, other story stiffness is 0.723105

    kN/m; the thickness and width of the

    raft are 1m and 4m, the section of the pile is 0.90.9m2, and the length of the pile is 15m, the elastic

    modulus of the concrete is 3.0104N/mm

    2; the soil around the pile is sand with moderate consistency, the

    elastic modulus of the soil: MPa86=E , the Poisson s' ratio of the soil: v=0.25,the angle of internal

    friction for soil: = 35 , and 3kN/m15000=hK .

    The time history of the horizontal ground acceleration employed is shown in Figure 4, with 3000points at equal spacing of 0.01 sec, and the peak value are 0.22g and 0.40g. This time history of the

    acceleration is translated to the time history of the displacement.

    Figure.3 4-storey and 3-spans frame supported on

    a pile group with the raft

    Figure.4 The time history of acceleration from Boston

    earthquake (0.22g)The result of analysis

    The seismic analysis for the frame using the before-mentioned model is done with the nonlinear pile

    foundation under the moderate (the peak of the acceleration is 0.22g) earthquake and large (the peak of

    the acceleration is 0.40g). Then this response is compared with the responses of the rigid foundation and

    the linear pile foundation to investigate the influence of the pile-soil interaction and nonlinear effect of the

    pile foundation on the super-structure.

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    The maximum interstory shear, interstory displacement and story displacement of the frame in different

    conditions of foundation are computed under the moderate earthquake (0.22g) and the large earthquake

    (0.40g). As shown in Table 1 the maximum interstory shear and the minimum story displacement are in

    the case of the rigid foundation. The interstory shear of the linear foundation condition is larger than that

    of the nonlinear foundation condition, and the story displacement of the linear foundation condition is

    smaller than that of the nonlinear foundation condition. The natural frequencies in different conditions of

    foundation are shown in Table 2. It can be seen that the natural frequency of the nonlinear foundationcondition is smallest.

    The time histories of the displacement of the top story in three different foundation conditions are shown

    in Figure 5 for the moderate earthquake (0.22g) and Figure 6 for the large earthquake (0.40g). From

    Figures 5 and 6, it can be illustrated that the maximum displacement of the top story is in case of the

    nonlinear foundation condition.Table 1. The maximum interstory shear,

    interstory displacement and story displacement of the frame

    Number of

    storymaximum interstory

    shear (kN) maximum interstory

    displacement )m( maximum story

    displacement )m(

    Rigid SSI Rigid SSI Rigid SSI

    1 1139.0887.0

    (1029.0) 0.02090.0163

    (0.0186) 0.05000.0559

    (0.0570)

    2 927.0813.3

    (913.1)0.0128

    0.0112

    (0.0126)0.0542

    0.0651

    (0.0599)

    3 750.8650.6

    (728.9)0.0107

    0.0093

    (0.0104)0.0644

    0.0731

    (0.0694)

    Moderate

    earthquake

    (0.22g)

    4 448.0420.6

    (444.8)0.0068

    0.0064

    (0.0067)0.0711

    0.0798

    (0.0750)

    1 20711996

    (19980.0381

    0.0367

    (0.037)0.0910

    0.1060

    (0.097)

    2 16861716

    (1660)0.0233

    0.0237

    (0.0229)0.0986

    0.1244

    (0.1219)

    3 13651288

    (1325)0.0195

    0.0184

    (0.0189)0.1171

    0.1421

    (0.1394)

    Large

    Earthquak

    e

    (0.40g)

    4 814.5789.98

    (808.8)0.0123

    0.0119

    (0.0122)0.1292

    0.1585

    (0.1449)

    annotationThe numerical value in () is the result in the case of the linear foundation condition.

    Table 2.Natural frequencies in different foundation conditions

    Condition of

    foundation

    Rigid SSI(linear) SSI(nonlinear)

    1 14.85 13.77 6.594

    2 18.36 16.89 11.66

    3 23.59 21.24 18.64

    4 24.51 24.34 24.26The contact states between the pile and the soil is shown in Figure 7 for the moderate earthquake (0.22g)

    and Figure 8 for the large earthquake (0.40g). In Figures 7 and 8, "1stat" = stands for that the contact state

    between the interfaces of the pile and soil is close, "3stat" = stands for that the contact state between the

    interfaces of the pile and soil is open, and "2stat" = stands for that the contact state between the

    interfaces of the pile and soil is slip. From Figures 7 and 8, it can be shown that the contact state between

    the pile and the soil changes from contact and slippage to separationwith seismic load under the moderate

    and large earthquakes.

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    (1) Nonlinear foundation condition (1) Nonlinear foundation condition

    (2) Linear foundation condition (2) Linear foundation condition

    (3) Rigid (3) Rigid

    Figure 5. The time history of the displacement of the

    top story under moderate earthquake

    Figure 6. The time history of the displacement of

    the top story under large earthquake

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    Figure 7.the contact state between the pile and soil

    under moderate earthquake

    Figure 8.the contact state between the pile and soil

    under large earthquake

    CONCLUSIONS

    Through the seismic response analysis of the frame supported on a pile group under the moderate andlarge earthquakes, the following conclusions can be summarized:

    1. The modified simplified nonlinear pile-soil-structure interaction (PSSI) model can consider the

    influence of the free-field on the super-structure directly, the nonlinear effect, and simplified the input

    method of Penzien model. Thus, it can be applied to engineering conventionally.

    2. The analysis shows that the contact state of the pile and the soil changes from contact and slippage to

    separation with the seismic load under the moderate and large earthquakes. So it is necessary to

    consider the contact nonlinear effect in PSSI system.

    3. In the case of nonlinear foundation condition, the seismic behavior is different from that in the rigid

    foundation condition and linear foundation condition.

    REFERENCES

    1. Penzien J, Scheffey C. F., Parmelee R. A. Seismic analysis of bridges on long piles. ASCE, 1964;

    90(EM3): 223-254.

    2. Hui Li, Soil-structure dynamic Interaction . ChongQing:PH.D. Dissertation in ChongQing JianzhuUniversity, 1998:63-69.

    3. Takewaki I. Inverse Stiffness Design of Shear-Flexural Building Models Including Soil-Structure

    Interaction . Engineering Structures, 1999;Vol.21: 1045- 1054.

    4. Xi-an Zhao, Construction and Structure Design of the tall buildings . China architecture & building

    press, 1992: 203-204.

    5. Technical Code for Building pile foundation. JGJ 94-94. Beijing: China architecture & building

    press, 1995: 251-252.

    6. Ren-li Hu. The analysis and design of the pile foundation of bridge. Beijing: China railroad press,

    1987: 86-161.

    7. Liam Finn W. D, Wu G, Thavaraj T. Soil-Pile-Structure Interaction Proceedings of Seismic Analysis

    and Design for Soil-Pile-Structure Interaction. Minneapolis, Minnesota: 1997:1-20.

    8. Wolf J. P. Foundation Vibration Analysis Using Simple Physical Models [M]. PTR Prentice Hall

    Englewood Cliffs. 1995.

    9. Song-tao Wang, Zi Cao. Modern aseismatic design method. Beijing: China architecture & building

    press, 1997: 58-162.10. Feng-Xia Wang. Seismic performance analysis of piles with raft -soil-structure interaction. Harbin:

    Master Thesis in Harbin Institute of Technology, 2002: 22-50.